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Metal estimation

Most of the stars of our sample have been selected from the H K BPS survey ( Beers, Preston Shectman [1], First, stars were selected from the weakness of their H H lines for the Balmer lines intensity on prism-objective Schmidt telescope plates. Then, the candidate stars were observed with a slit spectrograph in order to have a quantitative estimate of their metallicity. The survey has operated on about 7000 square degrees of the sky, mostly on the polar caps. It has supply a vast amount of metal-poor stars, with hundreds of them more metal-poor than the most metal-poor globular clusters. We selected from this sample stars with metallicities estimated to have [Fe/H] < -2.7. The actual metallicity histogram is given for the sample on fig. 1. [Pg.115]

Spectroscopy The WFI images were used to select samples of stars on the RGB in Scl to take spectra in the Ca II triplet region with VLT/FLAMES. This resulted in radial velocity measurements and metallicity estimates for more than 400 stars in Scl over the fields outlined in Fig. 1, of which 300 have a high membership probability. [Pg.215]

The NiO phase could be reduced to metallic Ni by hydrogen treatment (723 K, 1 h). The crystallite size of Ni metal (estimated from XRD pattern of the reduced sample) is similar to that of the NiO in the unreduced sample (e.g., for 7B, the Ni metal crystallite size is 8.2 nm). The textural characterization studies reveal that for the samples prepared by coprecipitation + digestion and hydrothermal synthesis (methods B and C) the pore sizes are in the mesopore range (2.9 to 6.8 nm) (Table 11.2). [Pg.189]

Let us consider an ideal metal with 2 x 10 cm valence electrons. For such a metal, estimate (a) its plasma frequency, (b) the optical density at 400 nm for... [Pg.147]

Excluding 155 million for HF and H2S04 alkylation catalysts. Including an estimated 160 million for noble metals. Estimated. [Pg.238]

Carbonyl metallates find their widest application as reagents for introducing electrophilic functionality to the metal centre, which is highly nucleophilic. Table 3.3 indicates nucleophilicities for a range of common carbonyl metallates estimated from conventional SN2 reaction rates with iodomethane. This illustrates their versatility in metal-carbon bond forming reactions however, as shown in Figure 3.6, this reactivity is not limited to carbon electrophiles but allows a wide range of metal-element bonds to be easily formed (see also reactions of metal carbonyls below). [Pg.50]

Tyson, W.R. and Miller, W.A. (1977) Siuface free energies of solid metal estimation from liquid surface tension measurements. Su. Sci., 62 (1), 267-276. Galanalds, I., BiMmayer, G., Bellini, V., Papanikolaou, N., Zeller, R., Bltigel, S., and Dederichs, P.H. (2002) Broken-bond rule for the surface energies of noble metals. Europhys. Lett., 58, 751-757. Galanalds, I., Papanikolaou, N., and Dederichs, P.H. (2002) Applicability of... [Pg.523]

Metal Estimated supply (years) Metal Estimated supply (years)... [Pg.17]

In the early theory of metals it was supposed that aU valence electrons in atoms become free and the metal structure is a lattice of cations immersed in an electron sea . Now it is known that only a part of the outer electrons of atoms are free, since the metallic radii are larger than those of cations (see Chap. 1). Some studies of electron density distribution in metals estimated the metallic/core radii ratio as 1 0.64 [117, 118]. The effective radii of the atomic cores in metallic structures are close to the bond radii of the same metals in crystalline compounds (see Chap. 1) which correspond to atoms with charges not exceeding 1. It should be noted that work functions of bulk metals are always smaller than the first ionization potentials of the corresponding atoms (see Sect. 1.1.2) and therefore there is no reason to suppose the ionization of two or more electrons from an atom. [Pg.68]

S-hydroxyquinoline, oxine, C9H7ON. Light brown needles, m.p. 15-16 C. Forms insoluble complexes with metals. The solubilities of the derivatives vary with pH, etc. and hence oxine is widely used in analysis. Used for estimating Mg, Al, Zn and many other metals. Many oxinates are extracted and the metal is estimated spectrophotometrically. Derivatives, e.g. 2-meIhyl tend to be specific, for, e.g.. Copper derivatives are used as fungicides. [Pg.212]

The most common technique for estimating thermal stability is called the Jet Fuel Thermal Oxidation Test (JFTOT). It shows the tendency of the fuel to form deposits on a metallic surface brought to high temperature. The sample passes under a pressure of 34.5 bar through a heated aluminum tube (260°C for Jet Al). After two and one-half hours, the pressure drop across a 17-micron filter placed at the outlet of the heater is measured (ASTM D 3241). [Pg.229]

Representative set of weldments was examined site welds (with pearlitic type weld metal) and two types of site weld repair zones with different welding technologies using Cr-Ni filler metals and Ni-based alloy. Results of AUGUR 4.2 inspection were compared with manual ultrasonic inspection ones in terms of defect detection, characterization, positioning and sizing in order to estimate correlation between these data. [Pg.195]

Using flaw visuahzation system data the strength and fracture mechanics estimations are carried out in accordance with defect assessment regulatory procedure M-02-91 [5]. Recently, the additions had been included in the procedure, concerning interpretation of expert flaw visualization sysf em data, computer modelling, residual stresses, in-site properties of metal, methods of fracture analysis. [Pg.196]

The Zond VD - 96 is intended for the detection of cracks, precipitates, inclusions etc. and corrosive defects with the preliminary estimation of their depth in various objects of magnetic and non - magnetic steels, non-ferrous and refractory metals and welds including coatings. [Pg.342]

But, with the use of digitization, 2D quantitative measurements are allowed for industrial radiography. These can be done by powerful tools, like estimation of defect extension, automatic segmentation, recognition of individual defects and image analysis (figure 7). For validation, results can be compared with destractive examination of metallic objects. [Pg.503]

In this paper, the performanees of laser-ultrasound are estimated in order to identify lacks of weld penetration. The laser-ultrasonic technique is applied to cylindrical metallic strucmres (few mm thick) in a single-sided control. The results obtained for different materials (gold-nickel alloy and tantalum) are presented by B-sean views for which the control configuration is discussed with regard to the thermal effects at the laser impact. This testing is performed for different lacks of weld penetration (up to 0.5 mm for a thickness of 2 mm) even in the presence of the weld bead, which corresponds to an actual industrial problem. [Pg.693]

The second model is a quantum mechanical one where free electrons are contained in a box whose sides correspond to the surfaces of the metal. The wave functions for the standing waves inside the box yield permissible states essentially independent of the lattice type. The kinetic energy corresponding to the rejected states leads to the surface energy in fair agreement with experimental estimates [86, 87],... [Pg.270]

The true area of contact is clearly much less than the apparent area. The former can be estimated directly from the resistance of two metals in contact. It may also be calculated if the statistical surface profiles are known from roughness measurements. As an example, the true area of contact. A, is about 0.01% of the apparent area in the case of two steel surfaces under a 10-kg load [4a]. [Pg.433]

These authors doubt that such interactions can be estimated other than empirically without fairly accurate knowledge of the structure in the interfacial region. Sophisticated scattering, surface force, and force microscopy measurements are contributing to this knowledge however, a complete understanding is still a long way off. Even submonolayer amounts of adsorbed species can affect adhesion as found in metals and oxides [74]. [Pg.454]

Figure Bl.22.1. Reflection-absorption IR spectra (RAIRS) from palladium flat surfaces in the presence of a 1 X 10 Torr 1 1 NO CO mixture at 200 K. Data are shown here for tluee different surfaces, namely, for Pd (100) (bottom) and Pd(l 11) (middle) single crystals and for palladium particles (about 500 A m diameter) deposited on a 100 A diick Si02 film grown on top of a Mo(l 10) single crystal. These experiments illustrate how RAIRS titration experiments can be used for the identification of specific surface sites in supported catalysts. On Pd(lOO) CO and NO each adsorbs on twofold sites, as indicated by their stretching bands at about 1970 and 1670 cm, respectively. On Pd(l 11), on the other hand, the main IR peaks are seen around 1745 for NO (on-top adsorption) and about 1915 for CO (tlueefold coordination). Using those two spectra as references, the data from the supported Pd system can be analysed to obtain estimates of the relative fractions of (100) and (111) planes exposed in the metal particles [26]. Figure Bl.22.1. Reflection-absorption IR spectra (RAIRS) from palladium flat surfaces in the presence of a 1 X 10 Torr 1 1 NO CO mixture at 200 K. Data are shown here for tluee different surfaces, namely, for Pd (100) (bottom) and Pd(l 11) (middle) single crystals and for palladium particles (about 500 A m diameter) deposited on a 100 A diick Si02 film grown on top of a Mo(l 10) single crystal. These experiments illustrate how RAIRS titration experiments can be used for the identification of specific surface sites in supported catalysts. On Pd(lOO) CO and NO each adsorbs on twofold sites, as indicated by their stretching bands at about 1970 and 1670 cm, respectively. On Pd(l 11), on the other hand, the main IR peaks are seen around 1745 for NO (on-top adsorption) and about 1915 for CO (tlueefold coordination). Using those two spectra as references, the data from the supported Pd system can be analysed to obtain estimates of the relative fractions of (100) and (111) planes exposed in the metal particles [26].
The polarization dependence of the photon absorbance in metal surface systems also brings about the so-called surface selection rule, which states that only vibrational modes with dynamic moments having components perpendicular to the surface plane can be detected by RAIRS [22, 23 and 24]. This rule may in some instances limit the usefidness of the reflection tecluiique for adsorbate identification because of the reduction in the number of modes visible in the IR spectra, but more often becomes an advantage thanks to the simplification of the data. Furthenuore, the relative intensities of different vibrational modes can be used to estimate the orientation of the surface moieties. This has been particularly useful in the study of self-... [Pg.1782]

A. (The gas phase estimate is about 100 picoseconds for A at 1 atm pressure.) This suggests tliat tire great majority of fast bimolecular processes, e.g., ionic associations, acid-base reactions, metal complexations and ligand-enzyme binding reactions, as well as many slower reactions that are rate limited by a transition state barrier can be conveniently studied with fast transient metliods. [Pg.2948]


See other pages where Metal estimation is mentioned: [Pg.306]    [Pg.142]    [Pg.72]    [Pg.64]    [Pg.557]    [Pg.325]    [Pg.164]    [Pg.74]    [Pg.146]    [Pg.199]    [Pg.77]    [Pg.217]    [Pg.270]    [Pg.29]    [Pg.306]    [Pg.142]    [Pg.72]    [Pg.64]    [Pg.557]    [Pg.325]    [Pg.164]    [Pg.74]    [Pg.146]    [Pg.199]    [Pg.77]    [Pg.217]    [Pg.270]    [Pg.29]    [Pg.27]    [Pg.57]    [Pg.145]    [Pg.275]    [Pg.227]    [Pg.791]    [Pg.258]    [Pg.270]    [Pg.433]    [Pg.434]    [Pg.591]    [Pg.712]    [Pg.922]    [Pg.1781]    [Pg.2714]   
See also in sourсe #XX -- [ Pg.169 , Pg.170 , Pg.171 , Pg.172 , Pg.173 ]




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